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Número de publicaciónUS7504704 B2
Tipo de publicaciónConcesión
Número de solicitud11/130,584
Fecha de publicación17 Mar 2009
Fecha de presentación17 May 2005
Fecha de prioridad
7 Mar 2003
También publicado como
Inventores
Cesionario original
Clasificación de EE.UU.
Clasificación internacional
Clasificación cooperativa
Clasificación europea
H01L 29/66M6T6F11E
H01L 29/78R
H01L 29/66M6T6F11B3
H01L 29/66M6T6F11D3
H01L 21/8234C
H01L 21/8238U
H01L 21/762C
H01L 29/10D2B4
H01L 21/8238C
Referencias
Enlaces externos
Shallow trench isolation process
US 7504704 B2
Resumen

A structure including a transistor and a trench structure, with the trench structure inducing only a portion of the strain in a channel region of the transistor.

Dibujos(19)
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Reclamaciones

1. A structure comprising:

a first transistor disposed over a first region of a substrate, the first transistor including:

a first source region and a first drain region disposed in a first portion of the substrate,

a first channel region disposed between the first source region and the first drain region, at least a portion of the first channel region located in a strained layer disposed over the substrate and lattice-mismatched to a proximate material inducing a first type of strain in the strained layer, the first channel region having the first type of strain, and

a first gate disposed above the first channel region and between the first source and first drain regions, the first gate comprising a conductive material; and

a first trench structure disposed in a trench,

wherein the trench is proximate at least one side of one of the first source region and the first drain region, the first trench structure inducing a portion of the first type of strain in the first channel region.

2. The structure of claim 1, wherein the strained layer comprises at least one of a group II, group III, group V, and group VI element.

3. A method for forming a semiconductor structure, the method comprising:

forming a first transistor over a first region of a substrate having a strained layer disposed thereover, the strained layer being lattice-mismatched to a proximate material inducing a first type of strain in the strained layer, the first transistor formed by:

defining a first source region and a first drain region in a first portion of the substrate,

defining a first channel region between the first source region and the first drain region, the first channel region having a first type of strain, at least a portion of the first channel region being disposed in the strained layer, and

forming a first gate above the first channel region and between the first source and first drain regions, the first gate comprising a conductive material;

forming a first trench proximate at least one side of one of the first source region and the first drain region; and

forming a first trench structure in the first trench, the first trench structure being tailored to induce only a portion of the first type of strain in the first channel region.

4. A method for forming a semiconductor structure, the method comprising:

providing a substrate;

forming a first transistor over a first region of the substrate by:

defining a first source region and a first drain region in a first portion of the substrate,

defining a first channel region between the first source region and the first drain region, the first channel region having a first type of strain, and

forming a first gate above the first channel region and between the first source and first drain regions, the first gate comprising a conductive material;

forming a first trench proximate at least one side of one of the first source region and the first drain region; and

forming a first trench structure in the first trench, the first trench structure being tailored to induce only a portion of the first type of strain in the first channel region,

wherein the gate induces at least a second portion of the first type of strain in the first channel region, and forming the first gate comprises (i) forming a polycrystalline semiconductor layer over the substrate and (ii) reacting the polycrystalline semiconductor layer with a metal, such that the first gate consists essentially of an alloy of the metal and the semiconductor layer.

5. The structure of claim 1, further comprising:

a dielectric layer disposed beneath the first channel region.

6. The structure of claim 1 wherein at least one of the first source region and the first drain region comprises a metal-semiconductor alloy, and the strain in the first channel region is induced by the metal-semiconductor alloy.

7. The structure of claim 1 wherein the first transistor is disposed in a chip, the structure further comprising:

a package housing the chip,

wherein the package induces strain in the first channel region.

8. The method of claim 3, further comprising:

forming a metal-semiconductor alloy over at least one of the first source region and the first drain region, the metal-semiconductor alloy tailored to induce the first type of strain in the first channel region.

9. The method of claim 4 further comprising, after forming the first gate, depositing an overlayer over the first gate, and annealing the first gate, wherein the first gate consists essentially of the alloy of the metal and the semiconductor layer.

10. A method for forming a semiconductor structure, the method comprising:

providing a substrate;

forming a first transistor over a first region of the substrate by:

defining a first source region and a first drain region in a first portion of the substrate,

defining a first channel region between the first source region and the first drain region, the first channel region having a first type of strain, and

forming a first gate above the first channel region and between the first source and first drain regions, the first gate comprising a conductive material;

forming a first trench proximate at least one side of one of the first source region and the first drain region;

forming a first trench structure in the first trench, the first trench structure being tailored to induce only a portion of the first type of strain in the first channel region;

disposing the first transistor in a chip; and

attaching the chip to a package,

wherein the package induces at least a portion of the first type of strain in the first channel region and the first type of strain is selected from the group consisting of tensile strain and compressive strain.

11. A method for forming a semiconductor structure, the method comprising:

providing a substrate comprising a strained layer having a first type of strain;

forming a masking layer over the substrate such that the masking layer exerts a second type of strain different from the first type of strain on the strained layer;

removing the masking layer over a first portion of the substrate; and

etching a trench in the first portion of the substrate,

wherein the first type of strain is opposite to the second type of strain.

12. The method of claim 11 wherein the masking layer comprises silicon nitride.

13. The method of claim 11, further comprising forming a pad oxide layer over the substrate prior to forming the masking layer.

14. A structure comprising:

a first transistor disposed over a first region of a substrate, the first transistor including:

a first source region and a first drain region disposed in a first portion of the substrate,

a first channel region disposed between the first source region and the first drain region, the first channel region having a first type of strain, and

a first gate disposed above the first channel region and between the first source and first drain regions, the first gate comprising a conductive material;

a first trench structure disposed in a trench; and

a first strain-inducing element that induces the first type of strain in the first channel region,

wherein the trench bounds the first source region and the first drain region, the first trench structure and the first strain-inducing element each inducing only a portion of the first type of strain in the first channel region, the first type of strain being selected from the group consisting of tensile and compressive strain.

15. The structure of claim 11 wherein the first type of strain is tensile and the second type of strain is compressive.

16. The structure of claim 11 wherein the first type of strain is compressive and the second type of strain is tensile.

17. The structure of claim 1, wherein the proximate material comprises an underlying layer.

18. The structure of claim 1, wherein the proximate material comprises a second material disposed in at least one of the first source and first drain regions.

19. The structure of claim 1, wherein the trench structure comprises a liner dielectric, a protective liner, and a dielectric material.

20. The structure of claim 3, wherein the proximate material comprises an underlying layer.

21. The structure of claim 3, wherein the proximate material comprises a second material disposed in at least one of the first source and first drain regions.

22. The structure of claim 3, wherein the trench structure comprises a liner dielectric, a protective liner, and a dielectric material.

Descripción
RELATED APPLICATION

This application is a continuation application of U.S. Ser. No. 10/794,010, filed Mar. 5, 2004, which claims the benefit of U.S. Provisional Application 60/452,794 filed Mar. 7, 2003, the entire disclosure of each of which is hereby incorporated by reference.

FIELD OF THE INVENTION

This invention relates generally to semiconductor structures and particularly to shallow trench isolation.

BACKGROUND

The formation of integrated circuits includes the definition of isolation regions to prevent parasitic current leakage between devices. Isolation techniques include the shallow trench isolation (STI) scheme that has increased the planarity and packing density of silicon very large scale integration (Si VLSI) devices, and has thus been the isolation scheme of choice since approximately the 0.25 micrometer (μm) technology node.

In a typical STI process, an active device area is protected by a pad oxide and a nitride overlayer, and isolation trenches are etched around the active device area. After the trench etch, a liner oxide is formed in each trench. This liner oxidation step serves several purposes. First, the oxidation eliminates any etch damage to a trench sidewall by consuming a small amount of the sidewall material. Second, the liner oxidation rounds the upper corners of the trench, minimizing the fringing fields that can result from sharp corners at the active area edge. If present, these fields form a parasitic, low-threshold voltage transistor at the active area edge that can degrade the subthreshold characteristics of the main device. Finally, because it is typically a thermal oxide, the liner oxide forms a high-quality interface between the Si trench sidewall and the deposited trench oxide. Interface traps, i.e., electrically active defects present at an oxide/semiconductor interface, are thereby minimized at this interface. The liner oxidation is often performed at high temperatures, i.e., >1000° C., and in an oxygen, i.e., dry ambient.

After the liner oxidation, a chemical vapor deposited (CVD) dielectric, such as silicon dioxide, is deposited over the entire substrate, filling the trenches. This CVD dielectric also covers the active device regions, and it should be selectively removed for device processing to continue. This is accomplished by planarizing the substrate, typically via chemical-mechanical polishing (CMP), using the silicon nitride layer over the active area as a stop layer. This process removes the dielectric from the active areas while retaining it in the isolation trenches. The nitride and pad oxide masking layers are then removed, resulting in a highly planar substrate with isolated device regions.

The formation of STI structures on silicon-germanium (SiGe) virtual substrates may be particularly challenging. SiGe virtual substrates are a platform for new generations of VLSI devices that exhibit enhanced performance in comparison to devices fabricated on bulk Si substrates. An important component of a SiGe virtual substrate is a layer of SiGe that has been relaxed to its equilibrium lattice constant, i.e., a lattice constant that is larger than that of Si. This relaxed SiGe layer may be formed directly on a Si substrate by, e.g., wafer bonding or direct epitaxy, or atop a relaxed graded SiGe layer, in which the lattice constant of the SiGe material has been increased gradually over the thickness of the layer. The SiGe virtual substrate can also incorporate buried insulating layers, echoing the structure of a semiconductor-on-insulator (SOI) wafer. In order to fabricate high-performance devices on these platforms, thin strained layers of Si, Ge, or SiGe are grown on the relaxed SiGe virtual substrates. The resulting biaxial tensile or compressive strain alters the carrier mobilities in the layers, enabling the fabrication of high speed and/or low power devices. Many issues and challenges arise when fabricating devices on SiGe rather than bulk Si substrates.

Forming an STI structure on a SiGe virtual substrate includes the etching and exposure of the underlying relaxed SiGe. Direct thermal liner oxidation of a trench etched in SiGe may be problematic and may result in a low-quality liner oxide. During liner oxidation, the Ge in the SiGe may be snowplowed ahead of an oxidation front, resulting in a pure silicon dioxide (SiO2) oxide layer atop a portion of a SiGe layer that is enriched in Ge content in comparison to the SiGe bulk material. Although in this case, the oxide itself has all of the properties of oxidized Si, it is proximate a layer of SiGe with an elevated Ge content. The presence of this elevated level of Ge at this interface may result in a very high density of interface traps. These interface traps may in turn result in increased subthreshold leakage, or in a shift in threshold voltage, for the active device, and are therefore undesirable.

If a trench is relied upon to induce all of the strain in a channel, the amount of strain that can be induced in the channel is limited. Too much trench-induced strain may produce defects, leading to problems with device operation.

SUMMARY

Trench structures, as well as other strain-inducing elements, are provided to induce strain in channel regions of transistors. This strain improves the performance of transistors, particularly those fabricated with small active area dimensions.

In accordance with an aspect of the present invention, interface trap density at an interface between a liner dielectric, such as an oxide, and a trench sidewall is decreased, i.e., at the point where the trench is defined in a SiGe virtual substrate. After the trench etch process is completed, a liner dielectric is formed. For example, a liner oxidation is performed such that the Ge present in the SiGe is not snowplowed ahead of the oxidation front. Instead, the Ge is incorporated into the liner oxide, leading to a decreased interface trap density and reduced subthreshold device leakage. The liner oxidation may take place in a wet, i.e., steam ambient and/or at a low temperature, i.e., <1000° C.

Since the liner oxide contains Ge incorporated during the oxidation process, it may be more susceptible to attack by etchants used during subsequent processing, e.g., wet cleans such as hydrofluoric acid (HF) or even rinses in deionized water. To protect the liner oxide from accelerated etching, a secondary protective liner may be used. This liner, preferably a dielectric material such as silicon nitride or silicon dioxide, may be deposited conformally over the initial liner oxide. The protective liner is selected to have a lower etch rate in wet etchants, such as HF, than the liner oxide. Since it may not contain Ge and may thus be less susceptible to etchants, this protective liner may preserve the integrity of the liner oxide during subsequent process steps. After the formation of the protective liner, the STI process is then continued as for Si substrates i.e., the trench is filled with a dielectric material such as high density plasma oxide.

In accordance with this invention, the interface between the liner dielectric and the trench sidewalls has a satisfactory integrity with a low interface trap density, e.g., less than 5×1011/cm2. Additionally, transistor off-state current (Ioff) is affected by the edge-leakage that occurs underneath the gate of the transistor. A low interface trap density in the portions of the STI disposed underneath the gate, therefore, is critical for obtaining a low Ioff. If the interface trap density is low, as enabled by this invention, sufficient leakage current cannot flow under the transistor gate to induce a high Ioff. In a transistor having a channel width of 1 μm, the Ioff may be less than 10−6 Ampere. In some embodiments, the off current may be less than 10−9 Ampere. This low device off current is achieved utilizing a novel STI process that has a large degree of process latitude. In some embodiments, because the Ge-containing liner oxide is protected by a protective liner, additional process steps will be similar to those employed in standard processes. The liner oxide's possible susceptibility to chemical attack will not place limits on subsequent process steps.

In an aspect of the invention, a masking material may be used during the formation of an STI structure, i.e., a trench structure, to induce a strain of a type different from a strain in a strained layer in which the trench structure is being defined.

In an aspect, the invention features a structure including a substrate, and a first transistor disposed over a first region of the substrate. The first transistor includes a first source region and a first drain region disposed in a first portion of the substrate, a first channel region disposed between the first source region and the first drain region, the first channel region having a first type of strain, and a first gate disposed above the first channel region and between the first source and first drain regions, the first gate including a material selected from the group of a doped semiconductor, a metal, and a metallic compound. A first trench structure is proximate at least one side of one of the first source region and the first drain region. The first trench structure induces only a portion of the first type of strain in the first channel region.

One or more of the following features may be included. A strained layer may be disposed over the substrate. The strained layer may include at least one of silicon and germanium. At least a portion of the first channel region may be disposed in the strained layer. A dielectric layer may be disposed over the substrate, and the strained layer may be disposed over and in contact with the dielectric layer. The first type of strain may be tensile. The first type of strain may be compressive. The substrate may include at least one of silicon and germanium. The substrate comprises at least one element other than silicon. The other element may be germanium.

A first cap layer may be disposed over a surface of the first transistor, and the strain in the first channel region may be induced by the first cap layer. The first cap layer may include silicon nitride. The strain in the first channel region may be induced by at least one of the first source region and the first drain region. The at least one of the first source region and the first drain region may include a second material having a larger lattice constant than a lattice constant of a semiconductor material disposed in at least one of the first channel region and an area proximate at least one of the first source region and the first drain region. The second material may include a material selected from the group including SiGe and Ge. The at least one of the first source region and the first drain region may include a second material having a smaller lattice constant than a lattice constant of a semiconductor material disposed in at least one of the first channel region and an area proximate at least one of the first source region and the first drain region. The second material may include a material selected from the group of SiGe, Si, and SiC.

The strain in the first channel region is induced by the first gate. The first gate may include material selected from the group of metal silicide, metal germanosilicide, and metal germanocide.

The structure may include a second transistor disposed over a second region of the substrate. The second transistor may include a second source region and a second drain region disposed in a second portion of the substrate, a second channel region disposed between the second source region and the second drain region, the second channel region having a second type of strain, and a second gate disposed above the second channel region and between the second source and second drain regions, the second gate including a material selected from the group of a doped semiconductor, a metal, and a metallic compound; and a second trench structure proximate at least one side of one of the second source region and the second drain region, the second trench structure inducing only a portion of the second type of strain in the second channel region. The first and second types of strain may be different.

The portion of the strain induced by the first trench structure may be approximately zero. The structure may include a first strain-inducing element, and a first epitaxial strained layer. The first channel region may be disposed within a portion of the first epitaxial strained layer and the first strain-inducing element may induce only a portion of the strain in the first channel region. The first strain-inducing element may include a first cap layer disposed over a surface of the first transistor. The first strain-inducing element may include the first gate. The first strain-inducing element may include at least one of the first source region and the first drain region.

In another aspect, the invention features a method for forming a semiconductor structure, the method including providing a substrate and forming a first transistor over a first region of the substrate. The first transistor may be formed by defining a first source region and a first drain region in a first portion of the substrate, defining a first channel region between the first source region and the first drain region, the first channel region having a first type of strain, and forming a first gate above the first channel region and between the first source and first drain regions, the first gate including a material selected from the group of a doped semiconductor, a metal, and a metallic compound. A trench structure may be formed proximate at least one side of one of the first source region and the first drain region, the first trench structure tailored to induce only a portion of the first type of strain in the first channel region.

One or more of the following features may be included. A second transistor may be formed over a second region of the substrate. The second transistor may be formed by defining a second source region and a second drain region in a second portion of the substrate, defining a second channel region between the second source region and the second drain region, the second channel region having a second type of strain, and forming a second gate above the second channel region and between the second source and second drain regions, the second gate including a material selected from the group of a doped semiconductor, a metal, and a metallic compound. A second trench structure is formed proximate at least one side of one of the second source region and the second drain region, the second trench structure tailored to induce only a portion of the second type of strain in the second channel region.

The first and second types of strain may be different. A first cap layer may be formed over a surface of the first transistor, the cap layer tailored to induce the first type of strain in the first channel region. At least a portion of the strain in the first channel region may be induced by at least one of the first source region and the first drain region. At least one of the first source region and the first drain region may include a second material having a larger lattice constant than a lattice constant of a semiconductor material disposed in at least one of the first channel region and an area proximate at least one of the first source region and the first drain region.

The at least one of the first source region and the first drain region may include a second material having a smaller lattice constant than a lattice constant of a semiconductor material disposed in at least one of the first channel region and an area proximate at least one of the first source region and the first drain region.

At least a portion of the strain in the first channel region may be induced by the first gate. The portion of the first type of strain the first trench structure is tailored to induce may be approximately zero. The first channel region may be defined in a portion of a first epitaxial strained layer.

A first strain-inducing element may be provided. The first strain-inducing element may include a first cap layer disposed over a surface of the first transistor. The first strain-inducing element may include the first gate. The first strain-inducing element may include at least one of the first source region and the first drain region.

BRIEF DESCRIPTION OF DRAWINGS

FIGS. 1-9 are a series of schematic cross-sectional views of a semiconductor structure illustrating a process for fabricating the structure;

FIGS. 10 a-10 e are schematic plan and cross-sectional views, of a device including the semiconductor structure illustrated in FIG. 9, with FIG. 10 b being taken along the line 10 b-10 b in FIG. 10 a; FIG. 10 c being taken along the line 10 c-10 c in FIG. 10 a; and FIGS. 10 d-10 e illustrating the semiconductor structure of FIG. 10 c after alternative processing steps; and

FIG. 11 is a cross-sectional view of a semiconductor structure including two transistors.

Like-referenced features represent common features in corresponding drawings.

DETAILED DESCRIPTION

In FIG. 1 a, which illustrates a structure amenable to use in connection with the present invention, a substrate 12 is made of a semiconductor, such as Si, Ge, or SiGe. A plurality of layers collectively indicated as 13 are formed on substrate 12. The plurality of layers 13 may include a relaxed graded buffer layer 14 disposed over substrate 12. Graded layer 14 includes, for example, SiGe having a grading rate of, for example, 10% Ge per μm of thickness, and a thickness T1 of, for example, 1-9 μm.

A relaxed layer 16 is disposed over graded SiGe layer 14. Relaxed layer 16 contains, for example, Si1-xGex wherein 0.1≦x≦0.9 and has a thickness T2 of, e.g., 0.2-2 μm. In some embodiments, Si1-xGex may include Si0.70Ge0.30 and T2 may be approximately 1.5 μm. Relaxed layer 16 may be substantially or fully relaxed, as determined by triple axis X-ray diffraction, and may have a threading dislocation density of <1×106 dislocations/cm2, as determined by etch pit density (EPD) analysis. Because threading dislocations are linear defects disposed within a volume of crystalline material, threading dislocation density may be measured as either the number of dislocations intersecting a unit area within a unit volume or the line length of dislocation per unit volume. Threading dislocation density therefore, may be expressed in either units of dislocations/cm2 or cm/cm3. Relaxed layer 16 may have a surface particle density of, e.g., less than about 0.3 particles/cm2. Further, relaxed layer 16 may have a localized light-scattering defect level of less than about 0.3 defects/cm2 for particle defects having a size (diameter) greater than 0.13 μm, a defect level of about 0.2 defects/cm2 for particle defects having a size greater than 0.16 μm, a defect level of about 0.1 defects/cm2 for particle defects having a size greater than 0.2 μm, and a defect level of about 0.03 defects/cm2 for defects having a size greater than 1 μm. Process optimization may enable reduction of the localized light-scattering defect levels to about 0.09 defects/cm2 for particle defects having a size greater than 0.09 μm and to 0.05 defects/cm2 for particle defects having a size greater than 0.12 μm.

Substrate 12, graded layer 14, and relaxed layer 16 may be formed from various material systems, including various combinations of group II, group III, group IV, group V, and group VI elements. For example, each of substrate 12, graded layer 14, and relaxed layer 16 may include a III-V compound. Substrate 12 may include gallium arsenide (GaAs), graded layer 14 and relaxed layer 16 may include indium gallium arsenide (InGaAs) or aluminum gallium arsenide (AlGaAs). These examples are merely illustrative, and many other material systems are suitable.

A strained semiconductor layer 18 is disposed over relaxed layer 16. Strained layer 18 may include a semiconductor such as at least one of a group II, a group III, a group IV, a group V, and a group VI element. Strained semiconductor layer 18 may include, for example, Si, Ge, SiGe, GaAs, indium phosphide (InP), and/or zinc selenide (ZnSe). Strained layer 18 may have a starting thickness T3 of, for example, 50-1000 angstroms (Å). In an embodiment, T3 may be approximately 200-500 Å.

Strained layer 18 may be formed by epitaxy, such as by atmospheric-pressure CVD (APCVD), low- (or reduced-) pressure CVD (LPCVD), ultra-high-vacuum CVD (UHVCVD), by molecular beam epitaxy (MBE), or by atomic layer deposition (ALD). Strained layer 18 containing Si may be formed by CVD with precursors such as dichlorosilane, silane, disilane, or trisilane. Strained layer 18 containing Ge may be formed by CVD with precursors such as germane or digermane. The epitaxial growth system may be a single-wafer or multiple-wafer batch reactor. The growth system may also utilize a low-energy plasma to enhance layer growth kinetics.

In an embodiment in which strained layer 18 contains substantially 100% Si, strained layer 18 may be formed in a dedicated chamber of a deposition tool that is not exposed to Ge source gases, thereby avoiding cross-contamination and improving the quality of the interface between strained layer 18 and relaxed layer 16. Furthermore, strained layer 18 may be formed from an isotopically pure precursor(s). Isotopically pure materials (e.g., Si or Ge) have better thermal conductivity than materials present as mixtures of atomic isotopes. Higher thermal conductivity may help dissipate heat from devices subsequently formed on strained layer 18, thereby maintaining the enhanced carrier mobilities provided by strained layer 18.

After formation, strained layer 18 has an initial misfit dislocation density of, for example, 0-105 cm/cm2. In an embodiment, strained layer 18 has an initial misfit dislocation density of approximately 0 cm/cm2. Because misfit dislocations are linear defects generally lying within a plane between two crystals within an area, they may be measured in terms of total line length per unit area. Misfit dislocation density, therefore, may be expressed in units of dislocations/cm or cm/cm2. In one embodiment, strained layer 18 may be tensilely strained, e.g., Si formed over SiGe. In another embodiment, strained layer 18 may be compressively strained, e.g., Ge formed over SiGe.

Strained layer 18 may have a surface particle density of, e.g., less than about 0.3 particles/cm2. As used herein, “surface particle density” includes not only surface particles but also light-scattering defects, and crystal-originated pits (COPs), and other defects incorporated into strained layer 18. Process optimization may enable reduction of the localized light-scattering defect levels to about 0.09 defects/cm2 for particle defects having a size greater than 0.09 μm and to 0.05 defects/cm2 for particle defects having a size greater than 0.12 μm. These surface particles may be incorporated in strained layer 18 during the formation of strained layer 18, or they may result from the propagation of surface defects from an underlying layer, such as relaxed layer 16.

In alternative embodiments, graded layer 14 may be absent from the structure. Relaxed layer 16 may be formed in various ways, and the invention is not limited to embodiments having graded layer 14. In other embodiments, strained layer 18 may be formed directly on substrate 12. In this case, the strain in layer 18 may be induced by lattice mismatch between layer 18 and substrate 12, induced mechanically, e.g., by the deposition of overlayers, such as Si3N4, or induced by thermal or lattice mismatch between layer 18 and a subsequently grown layer, such as a SiGe layer. In some embodiments, a uniform semiconductor layer (not shown), having a thickness of approximately 0.01-1.5 μm and comprising the same semiconductor material as substrate 12, is disposed between graded buffer layer 14 and substrate 12. This uniform semiconductor layer may be grown to improve the material quality of layers subsequently grown on substrate 12, such as graded buffer layer 14, by providing a clean, contaminant-free surface for epitaxial growth. In certain embodiments, relaxed layer 16 may be planarized prior to growth of strained layer 18 to eliminate the crosshatched surface roughness induced by graded buffer layer 14. (See, e.g., M. T. Currie, et al., Appl. Phys. Lett., 72 (14) p. 1718 (1998), incorporated herein by reference.) The planarization may be performed by a method such as CMP, and may improve the quality of a subsequent bonding process because it minimizes the wafer surface roughness and increases wafer flatness, thus providing a greater surface area for bonding.

Referring to FIG. 1 b, after planarization of relaxed layer 16, a relaxed semiconductor regrowth layer 20 including a semiconductor such as SiGe may be grown on relaxed layer 16, thus improving the quality of subsequent strained layer 18 growth by ensuring a clean surface for the growth of strained layer 18. Growing on this clean surface may be preferable to growing strained material, e.g., silicon, on a surface that is possibly contaminated by oxygen and carbon from the planarization process. The conditions for epitaxy of the relaxed semiconductor regrowth layer 20 on the planarized relaxed layer 16 may be chosen such that surface roughness of the resulting structure, including layers formed over regrowth layer 20, is minimized to ensure a surface suitable for, in some embodiments, subsequent high quality bonding for forming, e.g., a strained semiconductor-on-insulator (SSOI) structure.

In another embodiment, a compressively strained layer (not shown) may be disposed below or above strained layer 18. In such embodiment, the compressively strained layer includes Si1-yGey with a Ge content (y) higher than the Ge content (x) of relaxed Si1-xGex layer 16. The compressively strained layer may contain, for example, a Ge content wherein 0.3≦y≦1 and have a thickness of, e.g., 10-200 Å.

FIG. 1 c illustrates another type of structure amenable to use in connection with the present invention. Specifically, the structure is an SSOI substrate 22 having an insulator layer 24 disposed beneath strained layer 18. Insulator layer 24 may be a dielectric layer including an oxide, for example, SiO2. In an embodiment, dielectric layer 24 may include a material having a higher melting point (Tm) than that of pure SiO2, i.e., higher than 1700° C. Examples of such materials are silicon nitride (Si3N4), aluminum oxide, magnesium oxide, etc. Using dielectric layer 24 with a high Tm helps prevents possible relaxation of the transferred strained semiconductor layer 18 that may occur during subsequent processing, due to softening of the underlying dielectric layer 24 at temperatures typically used during device fabrication (approximately 1000-1200° C.). In such embodiment where strained layer 18 is formed directly on insulator layer 24, relaxed layer 16 and graded layer 14 may be absent from the structure. In another embodiment (not shown), the insulator layer 24 may be disposed directly beneath relaxed layer 16. In this case, graded layer 14 may be absent from the structure. The insulator layer 24 may have a thickness of, e.g., 200-3000 Å.

Referring to FIG. 2, a first masking layer 26, such as a pad silicon dioxide layer, hereinafter referred to as pad oxide 26, is formed over strained layer 18 by thermal growth or by a suitable deposition method such as low-pressure chemical vapor deposition (LPCVD). Pad oxide 26 may have a thickness T4 of, e.g., 50-200 Å. Subsequently, a second masking layer 28, such as a masking silicon nitride layer, is deposited over pad oxide 26 by a suitable deposition method such as LPCVD, high density plasma CVD, or plasma-enhanced chemical vapor deposition (PECVD). Masking layer 28 may be a dielectric material, e.g. silicon nitride or silicon oxynitride, and may be etched selectively with respect to underlying pad oxide 26.

Masking layer 28 may include a material selected to exert a type of strain different from the type of strain in strained layer 18. For example, in one embodiment, strained layer 18 may have a first type of strain, e.g., tensile strain, and masking layer 28 may have a second type of strain, e.g., compressive strain. More specifically, strained layer 18 may include tensilely strained silicon and masking layer 28 may include compressively strained silicon nitride. In another embodiment, strained layer 18 may be compressively strained, and masking layer 28 may be tensilely strained. More specifically, strained layer 18 may include compressively strained germanium, and masking layer 28 may include tensilely strained silicon nitride.

Mismatching the types of strain in masking layer 28 and strained layer 18 may help prevent relaxation of strained layer 18 during subsequent high temperature processing steps. In addition, although the thickness of pad oxide 26 may typically be selected to be large enough to buffer the underlying structure from strain exerted by masking layer 28, the thickness of pad oxide 26 may be reduced (e.g., to less than 200 Å, preferably less than 100 Å) to facilitate the exertion of strain by masking layer 28 on underlying layers. Masking layer 28 may have a thickness T5 of, for example, 500-2000 Å.

The strain of silicon nitride films grown by LPCVD at temperatures greater than approximately 700° C. may be selected by varying the silicon content of the nitride film. (See, e.g., S. Habermehl, J. Appl. Phys., 83 (9) p. 4672 (1998), incorporated herein by reference.) For example, LPCVD stoichiometric silicon nitride films (i.e., Si3N4) are typically tensilely strained, while silicon-rich nitride films (e.g., with a silicon volume fraction greater than 0.1-0.15, or with a Si/N atomic ratio greater than 0.75) are typically compressively strained. The silicon content of a nitride film formed by LPCVD may be varied by changes in the ratio of silicon and nitrogen precursors utilized in the growth process. For example, a nitride growth process performed at 850° C. and a pressure of 200 milliTorr (mTorr) utilizing dichlorosilane (SiCl2H2) as a silicon precursor and ammonia (NH3) as a nitrogen precursor will form a silicon-rich nitride when the ratio of dichlorosilane flow to the total gas flow is greater than approximately 0.85. For lower temperatures, the relative amount of dichlorosilane may need to be increased to form silicon-rich nitride films. Compressive silicon nitride films may have a refractive index greater than approximately 2.4, and tensile silicon nitride films may have a refractive index smaller than approximately 2.4. (See, e.g., M. Sekimoto, et al., J. Vac. Sci. Technol., 21 (4) p. 1017 (1982), incorporated herein by reference.)

In another embodiment, silicon nitride films for various strain levels may be formed by PECVD at deposition temperatures less than approximately 700° C. Variations in precursor gas ratio, RF power, dilution gas, and plasma excitation frequency may lead to strain variations in the final film. For example, for a PECVD process performed at 220° C., 200 Pascals pressure, 100 watts RF power, and helium dilution, a compressive silicon nitride film may be deposited when the ratio of silane flow to total gas flow (silane, ammonia, and nitrogen) is smaller than approximately 0.03. When this ratio is larger than approximately 0.03, a tensilely strained silicon nitride film may be deposited. (See, e.g., M. J. Loboda, et al., J. Mater. Res., 11 (2) p. 391 (1996), incorporated herein by reference.)

In an alternative embodiment, silicon nitride films of varying strain levels may be produced by high density plasma CVD (HDPCVD) in a process utilizing an inductively coupled plasma (ICP) source at temperatures less than 500° C. with precursors such as silane, ammonia, and nitrogen. The plasma used in this process may utilize noble gases such as argon or helium, which may also act as dilution gases in this process. The chuck power levels may be varied to tailor strain levels in silicon nitride films. For example, a process at 150° C. and 10 mTorr utilizing silane, ammonia, and helium gases (total gas flow of 40 standard cubic centimeters per minute (sccm)) and an ICP power of 800 watts may produce compressively strained silicon nitride films for RF chuck power levels less than approximately 40 watts and tensilely strained silicon nitride films for RF chuck power levels greater than approximately 40 watts. (See, e.g., J. W. Lee, et al., J. Electrochemical. Soc., 147 (4) p. 1481 (2000), incorporated herein by reference.)

Referring to FIG. 2 and also to FIG. 3, a photoresist layer is deposited over a top surface 30 of masking layer 28 and patterned to form a photoresist mask 32. Photoresist mask 32 defines an opening 34 over a region 36 of substrate 12 and layers 13 in which a trench structure 55 may be formed (see, e.g., trench structure 55 in FIG. 5 a). Opening 34 exposes a portion 37 of top surface 30 of masking layer 28 disposed over region 36.

After the definition of photoresist mask 32, a portion 38 of masking layer 28 exposed by photoresist layer 32 is removed, leaving behind masking layer portions 28 a, 28 b protected by photoresist mask 32 and exposing a portion 40 of pad oxide 26. Portion 40 of pad oxide 26 is then removed, leaving behind pad oxide portions 26 a, 26 b. In particular, exposed masking layer portion 38 may be removed by a suitable removal process such as a reactive ion etch (RIE) using gases such as a combination of nitrogen trifluoride, ammonia, and oxygen, or a combination of hydrogen bromide, chlorine, and oxygen. Pad oxide portion 40 may be removed by a wet etch that is selective to silicon, such as a hydrofluoric acid etch. The removal of pad oxide portion 40 exposes a portion 42 of strained layer 18. In an alternative embodiment, a first RIE etch may be to performed to remove portion 38 of masking layer 28, as well as portion 40 of pad oxide 26. This first RIE etch may not be selective to underlying semiconductor material, and may etch perhaps a few hundred Å into an underlying semiconductor material, e.g., strained layer 18. Then a second RIE etch step may be performed with a different chemistry and/or etch conditions, to remove ˜2500-4000 Å of underlying material, as described below with reference to formation of trench 50.

Referring to FIG. 3 and also to FIG. 4, a trench 50 is defined in strained layer 18 and relaxed layer 16. Trench 50 may be formed, for example, by a dry reactive ion etch. A two-step etch process may be used, with the strained layer 18 being etched during the first step with a gas such as chlorine and/or hydrogen bromide, and the relaxed layer 16 being etched during the second step with a gas such as chlorine and/or hydrogen bromide. The total gas pressure and/or the flow ratio of etch gases may differ between the steps of the two-step etch process. Trench 50 may have a depth d1 within a range of, for example, 3000-4000 Å, and a width w1 of less than depth d1, e.g., w1 may be approximately 1000 Å. In some embodiments, the width w1 of trench 50 may be larger than its depth d1, with w1 being as large as several micrometers. In some embodiments, depth d1 may be even deeper, e.g., in deep trench isolation processes. A sidewall 58 of trench 50 may be substantially vertical, i.e., forming an angle α of greater than approximately 80° with a plane parallel to a surface of the substrate. The bottom corners of trench 50 may be substantially rounded to facilitate subsequent filling with an isolation material. After the selective removal of portions 38, 40 of masking layer 28 and pad oxide 26 and the formation of trench 50, photoresist mask 32 may be removed by a stripping process such as a dry strip in an oxygen plasma.

Referring to FIG. 5 a, and also to FIG. 5 b, trench structure 55 is formed in trench 50. Forming the trench structure 55 may include lining trench sidewalls 58 a, 58 b and trench bottom portion 58 c with a first dielectric layer 72. First dielectric layer 72 may include an oxide, and it may be formed on any portion of strained layer 18 and relaxed layer 16 exposed in trench 50. First dielectric layer 72 may be e.g. 50-150 Å thick. In one embodiment, first dielectric layer 72 may include a nitrided oxide that may result in a lower interface state density than may be obtained with first dielectric layer 72 formed of pure silicon dioxide thermally grown on SiGe.

In one embodiment and referring to FIG. 5 a, first dielectric layer 72 may be a thermally grown oxide, formed, for example, by thermal growth in a conventional furnace, such as the ALPHA-8SE manufactured by Tokyo Electron (Austin, Tex.). This oxidation step may take place in a wet, i.e., steam ambient, and/or at a low temperature, i.e., <1000° C. Alternatively, first dielectric layer 72 may be formed by rapid thermal oxidation to reduce STI-module thermal budget. A suitable processing system is the RADIANCE CENTURA system manufactured by Applied Materials (Santa Clara, Calif.). In this embodiment, the oxidation step may further utilize plasma enhancement to increase the oxidation rate. The rapid thermal oxidation may take place in a wet, i.e., steam ambient. Because the rapid thermal oxidation time is limited, e.g., 5 minutes or less, the oxidation may take place at higher temperatures, i.e., >1000° C., although it may still be preferable to carry out the oxidation at a lower temperature, i.e., <1000° C. In other embodiments, first dielectric layer may be formed by thermal oxidation in a dry, e.g., oxygen, ambient or may be formed at elevated pressures, e.g., high-pressure oxidation (HIPOX).

These thermal oxidation processing parameters may permit the incorporation into the oxide of elements, including elements other than Si, disposed in substrate 12. For example, in some embodiments, substrate 12 with layers 13 may be a SiGe virtual substrate and first dielectric layer 72 may include Ge. The ratio of Ge to Si in first dielectric layer 72 may be substantially similar to the ratio of Ge to Si in a substrate portion 74 that includes relaxed layer 16 and strained layer 18. More specifically, first dielectric layer 72 may be an oxide in the form of Si1-xGexO2. Further, an interface 76 between first dielectric layer 72 and trench sidewalls 58 a, 58 b may have a satisfactory integrity with a low interface trap density, e.g., less than 5×1011/cm2.

In another embodiment and referring to FIG. 5 b, first dielectric layer 72 may include an oxide, such as SiO2, formed by a suitable deposition method such as LPCVD or PECVD. In this embodiment, first dielectric layer 72 may be pure SiO2, i.e., it may not include Ge. Because first dielectric layer 72 is deposited, the formation of first dielectric layer 72 does not substantially affect the composition of substrate portion 74 at interface 76 between first dielectric layer 72 and trench sidewalls 58 a, 58 b. More specifically, a first region 74 a of substrate portion 74 proximate the interface 76 may have a Ge concentration substantially similar to a Ge concentration in a second region 74 b of substrate portion 74 distal the interface 76. The interface 76 between first dielectric layer 72 and trench sidewalls 58 a, 58 b may have a satisfactory integrity with a low interface trap density, e.g., less than 5×1011/cm2. In some embodiments, deposition of first dielectric layer 72 may be followed by an oxidation step to further improve the integrity of interface 76.

Referring to FIG. 6, in some embodiments, trench structure 55 may include a secondary protective liner 78 formed proximate first dielectric layer 72. This protective liner 78, preferably a dielectric material such as silicon nitride or silicon dioxide, may be deposited conformally over first dielectric layer 72. Protective liner 78 may have a thickness T6 of, e.g., 50-500 Å. Because in some embodiments first dielectric layer 72 may contain Ge, it may be susceptible to attack by etchants used during subsequent processing, e.g., wet cleans such as hydrofluoric acid or even rinses in deionized water. Protective liner 78 may be selected to have a lower etch rate than first dielectric layer 72 in wet etchants such as hydrofluoric acid, or an RCA SC1 clean including water, hydrogen peroxide, and ammonium hydroxide. The formation of the secondary protective liner 78 may thus help to protect first dielectric layer 72 from accelerated etching, thereby preserving the integrity of first dielectric layer 72 during subsequent process steps. Protective liner 78 may also protect the sidewalls 58 a, 58 b of trench 50 from oxidation during subsequent process steps performed at elevated temperatures and/or in ambients containing oxygen. The volume expansion from such oxidation may result in unwanted compressive strain being induced in the region bounded by the trench structure or in the channel region of subsequently fabricated devices.

Materials and methods of forming dielectric layer 72 (and optionally protective liner 78) may be tailored to define trench structure 55 having the same type of strain as that in a particular layer of the substrate. For example, when strained layer 18 is compressively strained, dielectric layer 72 may be formed in a manner and of a material that will result in it also being compressively strained. In another embodiment, strained layer 18 may be tensilely strained, and dielectric layer 72 may be formed in a manner and of a material that will result in it also being tensilely strained.

In some embodiments, trench structure 55 may include both first dielectric 72 and protective liner 78, and the two layers may exert the same type of strain or different types of strain. Having different types of strain in first dielectric 72 and protective liner 78 may be advantageous. For example, when first dielectric 72 is formed in a steam ambient, compressive strain may be created in trench structure 55 and may affect device performance. Protective liner 78 may help to counteract this compressive strain by providing a tensilely strained layer. The total amount of strain of first dielectric 72 and protective liner 78 is preferably the same type of strain as the type of strain in one of the plurality of layers 13 on substrate 12, for example, strained layer 18.

Referring to FIG. 7, trench 50 may be filled with a fill material 80 selected to define a trench structure 55 having the same type of strain as that in one of the plurality of layers 13 disposed over substrate 12. In one embodiment, the fill material 80 is a dielectric, such as silicon dioxide. Fill material 80 may be deposited by, for example, LPCVD, PECVD, or HDPCVD, and may have a thickness sufficient to completely fill trench 50. Alternatively, fill material 80 may be deposited by a spin-on process, e.g., fill material 80 may be a spin-on-glass material such as an inorganic spin-on-glass based on polysilazane. A portion 82 of fill material 80 may be disposed outside trench 50.

In an embodiment in which it is desired that trench structure 55 induce tensile strain, fill material 80 may include an amorphous semiconductor, e.g., amorphous silicon. In a subsequent step (either an additional step, or during a further processing step), fill material 80 may be heated to a temperature above its amorphous-polycrystalline phase transition temperature by annealing or by irradiation with ultraviolet or laser energy. Depending on the method, this may include heating fill material 80 to a temperature higher than approximately 500-700° C. During the phase transition that takes place above its amorphous-polycrystalline phase transition temperature, fill material 80 contracts, inducing tensile strain in a region bounded by trench structure 55, e.g., in a channel region of a subsequently fabricated device.

In an alternative embodiment, fill material 80 has a thermal expansion coefficient greater than that of the material within which it is predominantly formed (i.e. strained layer 18, relaxed layer 16, or substrate 12) and it is deposited at elevated temperatures. Depending on the materials present in strained layer 18, relaxed layer 16, and substrate 12, fill material 80 may be selected to have a coefficient of thermal expansion greater than that of Si (2.6×10−6/° C.), Ge (5.8×10−6/° C.), or GaAs (6.86×10−6/° C.). In the case of trench 50 being formed predominately in SiGe, the coefficient of thermal expansion of the SiGe may be approximated as the weighted average of the coefficients of thermal expansion of Si and Ge. Because coefficients of thermal expansion for these materials tend to increase with temperature, fill material 80 may be chosen to have a coefficient of thermal expansion greater than 8×10−6/° C. In this embodiment, when fill material 80 is cooled to room temperature, it contracts more than the surrounding material, inducing tensile strain in a region bounded by trench structure 55, e.g., in the channel region of a subsequently fabricated device. A material suitable for use as fill material 80 may be zinc-alumina-silicate glass.

In another embodiment, fill material 80 is not fully densified, e.g., fill material 80 may include low temperature oxide (LTO), medium temperature oxide (MTO), or silicon dioxide deposited from a tetraethylorthosilicate (TEOS) precursor. An anneal at a temperature above the deposition temperature, e.g., above 700° C., may cause fill material 80 to densify, i.e., contract, thereby inducing tensile strain in the region bounded by trench structure 55, e.g., in the channel region of a subsequently fabricated device. Such a densification anneal is preferably performed at a temperature sufficiently low, e.g., below 1100-1200° C., to prevent strain relief by flow of fill material 80.

In an embodiment, trench structure 55 induces compressive strain, and fill material 80 with a coefficient of thermal expansion smaller than that of the surrounding material may be deposited at elevated temperature. For example, when the surrounding material is predominantly silicon, the fill material 80 may be silicon dioxide. Thus, when fill material 80 is cooled to room temperature, it contracts less than the surrounding material, inducing compressive strain in the region bounded by trench structure 55, e.g., in the channel region of a subsequently fabricated device. In an alternative embodiment, fill material 80 may induce tensile strain as-deposited and may be densified or annealed at high temperatures, e.g., above 900° C. Flow of fill material 80 at such high temperatures may result in compressive strain being induced by fill material 80 after cooling. In another embodiment, compressive silicon dioxide may be deposited by PECVD. In an alternative embodiment, protective liner 78 may be absent in trench 50, and an oxidation step may be performed after filling the trench with fill material 80. Such oxidation is accompanied by a volume expansion which may further induce compressive strain in the region bounded by trench structure 55, e.g., in the channel region of a subsequently fabricated device.

Referring to FIG. 7 and also to FIG. 8, portion 82 of fill material 80 disposed outside trench 50 is removed, e.g., by CMP.

Referring to FIG. 8 and also to FIG. 9, remaining masking layer portions 28 a, 28 b and pad oxide portions 26 a, 26 b are removed, exposing a top surface 90 of strained layer 18, and leaving trench 50 filled with fill material 80, liner oxide 72, and in some embodiments, protective liner 78. Masking layer portions 28 a, 28 b may be removed by a removal process such as RIE using gases such as a combination of nitrogen trifluoride, ammonia, and oxygen, or a combination of hydrogen bromide, chlorine, and oxygen. Pad oxide portions 28 a, 28 b may be removed by a wet etch that is selective to silicon, such as a hydrofluoric acid etch. After removal of masking layer portions 28 a and 28 b and pad oxide portions 26 a and 26 b, a portion of fill material 80 may extend above top surface 90.

Referring to FIGS. 10 a-10 c, a structure 100 may include first and second parallel isolation trench structures 55 a, 55 b proximate a first source region 102 and a first drain region 104 of a first transistor 106. A first channel region 108 may be disposed between the first source and drain regions 102, 104. First channel region 108 may have a first type of strain. In some embodiments, the first type of strain may be tensile. In other embodiments, the first type of strain may be compressive. At least a portion of the first channel region 108 may be disposed in strained layer 18. A first gate 110 may be disposed above the channel region 108 and between the source and drain regions 102, 104. Gate 110 may be connected to a gate contact 1112. A first gate dielectric layer 114 may be formed between gate 110 and channel region 108. First gate 110 and first gate dielectric layer 114 may be collectively referred to as a first gate structure 116. A first and a second sidewall spacer 120, 122 may be formed proximate gate structure 116.

First transistor 106 may be formed on layers 13 disposed over substrate 12. As discussed above with reference to FIG. 1 a, layers 13 may include, for example, graded layer 14, relaxed layer 16, and strained layer 18. In other embodiments, first transistor 106 may be formed on an SSOI substrate 22, as shown in FIG. 1 c. Source region 102, channel region 108, and drain region 104 may be formed in a portion of the SSOI substrate 22, for example, in a portion of strained layer 18.

Source and drain regions 102, 104 may be formed by, e.g., ion implantation of either n-type or p-type dopants. Gate 110 may be formed of a conductive material, such as doped semiconductor, e.g., polycrystalline Si or polycrystalline SiGe; a metal, e.g., titanium (Ti), tungsten (W), molybdenum (Mo), tantalum (Ta), nickel (Ni), or iridium (Ir); or metallic compounds, e.g., titanium nitride (TiN), titanium silicon nitride (TiSiN), tungsten nitride (WN), tantalum nitride (TaN), tantalum silicide (TaSi), nickel silicide (NiSi), or iridium oxide (IrO2), that provide an appropriate workfunction. The gate dielectric layer 114 may be formed on strained layer 18 by, for example, growing a SiO2 layer by thermal oxidation. Alternatively, gate dielectric layer 114 may include a high-k material with a dielectric constant higher than that of SiO2, such as ZrO2, Al2O3, HfO2, HfSiON, or HfSiO4. In some embodiments, gate dielectric layer 114 may be a stacked structure, e.g., a thin SiO2 layer capped with a high-k material.

First and second trench structures 55 a, 55 b confine carriers (not shown), such as holes or electrons generated during operation of first transistor 106, within a region 124 having an outer semiconductor/insulating boundary 126 defined by first and second trench structures 55 a, 55 b and by adjacent third and fourth trench structures 55 c, 55 d. By confining carriers to region 124, trench structures 55 a-55 d help prevent further migration of the carriers, and thereby prevent leakage currents between first transistor 106 and other devices (not shown). The shallow trench isolation provided by first, second, third, and fourth trench structures 55 a-55 d is inadequate if the edge-leakage current associated with a high interface trap density at the semiconductor/insulating boundary 126 is sufficient to significantly increase the off-state current (Ioff) of transistor 106. On the other hand, this isolation suffices if the edge-leakage current associated with a low interface trap density at the semiconductor-trench boundary 126 ensures a low Ioff for first transistor 106. Ioff is affected by the edge-leakage that occurs underneath gate 110. A low interface trap density in the portions of boundary 126 disposed underneath gate 110, therefore, is critical for obtaining a low Ioff. If the interface trap density in boundary 126 underneath gate 110 is low, leakage current cannot flow under gate 110 sufficiently to induce a high Ioff. The Ioff may be less than 10−6 Ampere. In some embodiments, the off current is less than 10−9 Ampere.

Trench structures 55 a-55 d may include a first dielectric layer 72, and optionally a second protective liner 78. Parameters for forming trench structures 55 a-55 d may be selected such that one or more of the trench structures 55 a-55 d induces only a portion of the strain in channel region 108, but not the entire strain in channel region 108. For example, in an embodiment, channel region 108 may be compressively strained, and trench structures 55 a-55 d may be formed in a manner and of materials such that the trench structures 55 a-55 d are also compressively strained, and induce only a portion of the compressive strain in channel region 108. In another embodiment, channel region 108 may be tensilely strained, and trench structures 55 a-55 d may be formed in a manner and of materials such that the trench structures 55 a-55 d are also tensilely strained, and induce only a portion of the tensile strain in channel region 108. The portion of strain induced by trench structures 55 a-55 d may be between 0-99.9% of the strain in channel region 108.

As used herein, the term “active area length” refers to the dimension of the active device area bounded by trench structures 55 a-55 d parallel to the current flow and perpendicular to the gate. Referring to FIG. 10 a, the active area length is along the 10 c-10 c line. The term “active area width” refers to the dimension of the active area bounded by trench structures 55 a-55 d parallel to the gate and perpendicular to the direction of the current flow. With reference to FIG. 10 a, the active area width is along the 10 b-10 b line.

The use of trench structures to induce a portion of the strain in channel region 108 rather than inducing strain of the opposite type (e.g., inducing tensile strain in a compressively strained channel) may result in superior device performance, particularly when the dimensions of the active device area are scaled to small sizes. For example, device performance may be improved when the active area length is smaller than approximately 1 μm and/or the active area width is smaller than 0.5 μm.

As discussed above, in some embodiments, the strain in channel region 108 may arise from lattice mismatch between strained layer 18 and the underlying layers. In other embodiments, strained layer 18 may be a surface portion of substrate 12 upon which a transistor is fabricated. In such embodiments, the strain in channel region 108 may be induced by another structure, for example, a strain-inducing element 128, introduced during device fabrication. The strain in channel region 108 may be predominantly uniaxial. In other embodiments, the strain may be induced along multiple directions, e.g., the strain may be biaxial strain or hydrostatic strain.

As noted above, in some embodiments, a portion of the strain in channel region 108 may be induced by trench structures 55 a-55 d. In an embodiment, the portion of the strain induced in channel region 108 by trench structures 55 a-55 d may be approximately zero, and the strain in channel region 108 may be induced by other structures, for example, a strain-inducing element 128, introduced during device fabrication.

Various approaches may be used to tailor the strain induced by trench structures 55 a-55 d so that the induced strain is approximately zero. For example, the fill material in the trench structures 55 a-55 d may be selected to have a coefficient of thermal expansion to be approximately the same as the material surrounding the trenches 50, e.g., the fill material may include silicon when the trench is formed in a silicon substrate. Alternatively, the fill material may include two materials, with a first material having strain that is opposite to the strain of a second material.

With continued reference to FIG. 10 c, in one embodiment, the strain in first channel region 108 is induced by a first cap layer 130, such as a layer used as an etch stop during contact metallization. Cap layer 130 may be conformally disposed over the entire device structure 100, e.g., over a surface 132 of first transistor 106, and may be formed from a dielectric material, e.g., silicon nitride, processed to induce tensile or compressive strain in channel region 108. In an embodiment, cap layer 130 includes silicon nitride that may be processed to induce strain as previously described in the discussion of masking layer 28. Additionally, cap layer 130 may be implanted with atoms, e.g., Si or Ge atoms, to tailor the strain level induced in the channel region 108. In another embodiment, the strain in channel region 108 may be induced by the implantation of a gaseous species, e.g., hydrogen, oxygen, helium, or other noble gas, into gate 110 or into a region below channel region 108.

Gate 110 may also induce strain in channel region 108 if gate 110 is composed completely or nearly completely of a metal silicide, metal germanosilicide, or metal germanocide, e.g., nickel silicide (NiSi), nickel germanosilicide (NiSiGe), or nickel germanocide (NiGe). The reaction between the metal and the gate polycrystalline silicon, polycrystalline silicon-germanium, or polycrystalline germanium may result in a volumetric change that may induce strain in channel region 108 after processing. In an alternative embodiment, strain in gate 110 may be induced by deposition of an overlayer, e.g., an oxide, and annealing prior to complete or incomplete silicidation of the gate. Gate 110 may include a semiconductor material that has been amorphized, e.g., by an ion implantation step, and may undergo an amorphous-crystalline phase transition (and accompanying volumetric change) during a subsequent anneal. The presence of an overlayer during such an anneal may result in a strain being induced in channel region 108, even after the overlayer is removed and the gate is silicided.

With reference to FIGS. 10 d-10 e, in another embodiment, the strain in channel region 108 may be induced by the replacement of a portion of the semiconductor material in source region 102 and drain region 104, with a second material having a lattice constant different from that of the semiconductor material disposed in the channel region 108 or in an area 140 proximate at least one of the first source region 102 and first drain region 104. For example, first and second recesses 144, 148 may be defined in source region 102 and drain region 104 that include Si (in which case channel region 108 also includes Si), as described in, e.g., U.S. Pat. Nos. 6,651,273 and 6,621,131, incorporated by reference herein. Recesses 144, 148 may be filled with a second material 150 with a lattice constant larger than that of Si, such as SiGe, thereby inducing compressive strain in channel region 108. Alternatively, recesses 144, 148 in source region 102 and drain region 104 that include Si may be etched and refilled with second material 150 with a smaller lattice constant, such as silicon carbide (SiC), thereby inducing tensile strain in channel region 108. For source, drain, and channel regions that include SiGe, the refill second material 150 may be Ge or SiGe with a higher Ge content for inducing compressive strain or Si or SiGe with a lesser Ge content for inducing tensile strain. Area 140 may be, for example, a portion of relaxed layer 16 and/or a portion of strained layer 18. In an embodiment, first transistor 106 is formed on a bulk semiconductor substrate 12, and area 140 may include a portion of the bulk semiconductor substrate 12.

In another embodiment, strain in channel region 108 may also be induced predominantly by a silicided region of source region 102 and/or drain region 104. Volumetric changes during the reaction of the silicide metal with the semiconductor material in source region 102 or drain region 104 may cause strain to be induced in channel region 108. Such metals may include titanium, nickel, cobalt, platinum or other suitable metals. In such embodiments, source region 102 and drain region 104 may not be etched and refilled with alternative semiconductor materials.

In another embodiment, strain-inducing element 128 may be introduced during back-end metallization steps or during die-level packaging of a chip including first transistor 106. For example, strain-inducing element 128 could be the package to which the chip is attached after the completion of device fabrication. Such a package can be engineered, e.g., deformed or strained, to induce strain across an entire chip along one or more directions, thereby inducing strain in channel region 108. For such embodiments, bulk semiconductor substrate 12 may have a reduced thickness, e.g., due to removal of material by backside grinding. In another embodiment, strain-inducing element 128 could be a metallization layer or a dielectric layer between metal wiring layers deposited and/or processed in a manner such that strain is induced in channel region 108.

The methods described herein by which strain is induced in channel region 108 may be used in combination with the epitaxial strained layer 18 described above, and/or with SSOI or SOI wafers.

Referring to FIG. 11, a structure 200 may include a first transistor 106 and a second transistor 106′. The first transistor 106 may be disposed over a first region of substrate 12, for example, over a first region 202 of strained layer 18. Trench structures 55 a and 55 b may be formed proximate first source region 102 and first drain region 104. First source region 102 and first drain region 104 may, in turn, be disposed in a first portion of the substrate, for example, in a first portion 204 of strained layer 18. The second transistor 106′ may be disposed over a second region of substrate 12, for example, over a second region 202′ of strained layer 18. The second transistor 106′ may include a second source region 102′ and a second drain region 104′ disposed in a second portion of the substrate, for example, in a second portion 204′ of strained layer 18. The second transistor 106′ also may include a second channel region 108′ disposed between second source region 102′ and second drain region 104′. In some embodiments, second channel region 108′ may be tensilely strained. In other embodiments, second channel region 108′ may be compressively strained. A second gate 110′ may be disposed over second channel region 108′ and between second source region 102′ and second drain region 104′. The second gate 110′ may include a material such as a doped semiconductor, a metal, and a metallic compound. A second gate dielectric 114′ may be disposed between second gate 110′ and second channel region 108′.

A second trench structure 55 a′ may be formed proximate at least one side of second source region 102′ or second drain region 104′. A second pair of trench structures including trench structures 55 a′, 55 b′ may be formed proximate second source region 102′ and second drain region 104′. In an embodiment, second channel region 108′ may be compressively strained, and trench structures 55 a′, 55 b′ may be formed in a manner and of materials such that trench structures 55 a′, 55 b′ are also compressively strained, and induce a portion of the compressive strain in second channel region 108′. In another embodiment, second channel region 108′ may be tensilely strained, and trench structures 55 a′, 55 b′ may be formed in a manner and of materials such that trench structures 55 a′, 55 b′ are also tensilely strained, and induce a portion of the tensile strain in second channel region 108′.

The first channel region 108 and the second channel region 108′ may have the same or different types of strain. For example, in one embodiment, first channel region 108 may be compressively strained, while second channel region 108′ is tensilely strained. In this embodiment, trench structures 55 a, 55 b may be formed in a manner and of materials such that trench structures 55 a and 55 b are compressively strained, and induce a portion of the compressive strain in first channel region 108. Trench structures 55 a′, 55 b′ may be formed in a manner and of materials such that trench structures 55 a′, 55 b′ are tensilely strained, and induce a portion of the tensile strain in second channel region 108′.

In the case of first channel region 108 and second channel region 108′ having different types of strain, it may be advantageous in terms of process simplicity for trench structures 55 a, 55 b, 55 a′, 55 b′ to induce approximately no strain on channel regions 108 and 108′. In this case, the strain in strained layer 18 may be augmented with another strain-inducing technique described above, e.g., cap layer 130, strain-inducing gate 110, or etched and refilled source and drain regions 102 and 104. In an embodiment, first transistor 106 could include first channel region 108 in strained layer 18 that is tensilely strained, cap layer 130 that induces tensile strain, and trench structures 55 a, 55 b that induce little or no strain on first channel region 108. Second transistor 106′ could include second channel region 108′ in strained layer 18 that is compressively strained, source and drain regions 102′, 104′ comprising a material with a larger lattice constant than that of surrounding material (at least one of strained layer 18 and relaxed layer 16) and hence inducing compressive strain in second channel region 108′, and trench structures 55 a′, 55 b′ that induce little or no strain on second channel region 108′. These methods may also be utilized on SSOI substrates.

The use of these composite techniques to cooperatively induce the strain in channel region 108 rather than inducing strain of opposite types (e.g., inducing tensile strain in a compressively strained channel) may result in superior device performance, particularly when the dimensions of the active device area are scaled to small sizes. For example, device performance may be improved when the active area length is smaller than approximately 1 μm and/or the active area width is smaller than 0.5 μm.

In some embodiments, either or both of the gates of transistors 106, 106′ may be oriented along crystallographic directions offset from the customary in-plane [110] direction. For example, a transistor gate may be aligned to an in-plane [100] direction on a (100) Si wafer. In other embodiments, a substrate having a surface other than the customary (100) surface may be used in the manufacture of transistors 106, 106′. For example, a substrate with a (110) or (111) surface may be used. For the case of a SOI or SSOI substrate, a layer above the insulating layer may have an in-plane rotation with respect to an underlying substrate (i.e., the crystallographic directions in the layer may be different from that of the substrate) or may have surface crystallographic planes other than those of the underlying substrate. For example, a semiconductor layer may be rotated 45° in-plane prior to bonding to form an SOI or SSOI substrate. Alternatively, a semiconductor (strained or unstrained) may be formed with an alternative surface crystallographic plane (e.g., (110) or (111)) and bonded to a handle wafer (e.g., with a (100) surface).

Embodiments of this invention may also be applicable to transistors with multiple or wrap-around gates. Examples of these include fin-FETs, tri-gate FETs, omega-FETs, and double-gate FETs (the channels of which may be oriented horizontally or vertically).

The invention may be embodied in other specific forms without departing from the spirit or essential characteristics thereof. The foregoing embodiments are therefore to be considered in all respects illustrative rather than limiting on the invention described herein.

Citas de patentes
Patente citada Fecha de presentación Fecha de publicación Solicitante Título
US401004527 Abr 19761 Mar 1977Ruehrwein; Robert A.Process for production of III-V compound crystals
US435489824 Jun 198119 Oct 1982Bell Telephone Laboratories, IncorporatedMethod of preferentially etching optically flat mirror facets in InGaAsP/InP heterostructures
US44117349 Dic 198225 Oct 1983Rca CorporationEtching of tantalum silicide/doped polysilicon structures
US452266212 Ago 198311 Jun 1985Hewlett-Packard CompanyCVD lateral epitaxial growth of silicon over insulators
US454795628 Mar 198322 Oct 1985Bouadma; NoureddineProcess for producing a semiconductor laser with several independent wavelengths and laser obtained by this process
US464985919 Feb 198517 Mar 1987The United States Of America As Represented By The United States Department Of EnergyReactor design for uniform chemical vapor deposition-grown films without substrate rotation
US467507431 Jul 198523 Jun 1987Matsushita Electric Industrial Co., Ltd.Method of manufacturing semiconductor device
US47107881 Dic 19861 Dic 1987Licentia Patent-Verwaltungs-GmbhModulation doped field effect transistor with doped Si.sub.x Ge.sub.1-x -intrinsic Si layering
US471768119 May 19865 Ene 1988Texas Instruments IncorporatedMethod of making a heterojunction bipolar transistor with SIPOS
US474944111 Dic 19867 Jun 1988General Motors CorporationSemiconductor mushroom structure fabrication
US475547813 Ago 19875 Jul 1988International Business Machines CorporationMethod of forming metal-strapped polysilicon gate electrode for FET device
US476424620 Ago 198716 Ago 1988American Telephone And Telegraph Company, At&T Bell LaboratoriesBuried undercut mesa-like waveguide and method of making same
US477751726 Nov 198511 Oct 1988Fujitsu LimitedCompound semiconductor integrated circuit device
US478661531 Ago 198722 Nov 1988Motorola Inc.Method for improved surface planarity in selective epitaxial silicon
US480353929 Mar 19857 Feb 1989International Business Machines CorporationDopant control of metal silicide formation
US485798614 Jul 198615 Ago 1989Kabushiki Kaisha ToshibaShort channel CMOS on 110 crystal plane
US496350624 Abr 198916 Oct 1990Motorola Inc.Selective deposition of amorphous and polycrystalline silicon
US49690313 Feb 19836 Nov 1990Hitachi, Ltd.Semiconductor devices and method for making the same
US49874626 Ene 198722 Ene 1991Texas Instruments IncorporatedPower MISFET
US499097927 Abr 19895 Feb 1991Eurosil Electronic GmbhNon-volatile memory cell
US499777620 Jun 19905 Mar 1991International Business Machines Corp.Complementary bipolar transistor structure and method for manufacture
US501368129 Sep 19897 May 1991The United States Of America As Represented By The Secretary Of The NavyMethod of producing a thin silicon-on-insulator layer
US503434816 Ago 199023 Jul 1991International Business Machines Corp.Process for forming refractory metal silicide layers of different thicknesses in an integrated circuit
US508987227 Abr 199018 Feb 1992North Carolina State UniversitySelective germanium deposition on silicon and resulting structures
US509176718 Mar 199125 Feb 1992At&T Bell LaboratoriesArticle comprising a lattice-mismatched semiconductor heterostructure
US510894627 Jul 199028 Abr 1992Motorola, Inc.Method of forming planar isolation regions
US51555716 Ago 199013 Oct 1992The Regents Of The University Of CaliforniaComplementary field effect transistors having strained superlattice structure
US51660843 Sep 199124 Nov 1992Motorola, Inc.Process for fabricating a silicon on insulator field effect transistor
US517758310 Ene 19915 Ene 1993Kabushiki Kaisha ToshibaHeterojunction bipolar transistor
US519868920 May 199130 Mar 1993Fujitsu LimitedHeterojunction bipolar transistor
US52022841 Dic 198913 Abr 1993Hewlett-Packard CompanySelective and non-selective deposition of Si.sub.1-x Ge.sub.x on a Si subsrate that is partially masked with SiO.sub.2
US520786430 Dic 19914 May 1993Bell Communications ResearchLow-temperature fusion of dissimilar semiconductors
US520818212 Nov 19914 May 1993Kopin CorporationDislocation density reduction in gallium arsenide on silicon heterostructures
US521211026 May 199218 May 1993Motorola, Inc.Method for forming isolation regions in a semiconductor device
US521211223 May 199118 May 1993At&T Bell LaboratoriesSelective epitaxy of silicon in silicon dioxide apertures with suppression of unwanted formation of facets
US521792315 Ene 19928 Jun 1993Kabushiki Kaisha ToshibaMethod of fabricating a semiconductor device having silicided source/drain regions
US522141324 Abr 199122 Jun 1993At&T Bell LaboratoriesMethod for making low defect density semiconductor heterostructure and devices made thereby
US522570330 May 19916 Jul 1993Mitsubishi Denki Kabushiki KaishaDual field effect transistor structure employing a single source region
US52408761 Jun 199231 Ago 1993Harris CorporationMethod of fabricating SOI wafer with SiGe as an etchback film in a BESOI process
US524119713 Sep 199131 Ago 1993Hitachi, Ltd.Transistor provided with strained germanium layer
US524284727 Jul 19927 Sep 1993North Carolina State University At RaleighSelective deposition of doped silion-germanium alloy on semiconductor substrate
US524320730 Nov 19927 Sep 1993Texas Instruments IncorporatedMethod to integrate HBTs and FETs
US525044517 Ene 19925 Oct 1993Texas Instruments IncorporatedDiscretionary gettering of semiconductor circuits
US525487319 Oct 199219 Oct 1993Motorola, Inc.Trench structure having a germanium silicate region
US528508618 Jun 19928 Feb 1994At&T Bell LaboratoriesSemiconductor devices with low dislocation defects
US529143912 Sep 19911 Mar 1994International Business Machines CorporationSemiconductor memory cell and memory array with inversion layer
US52945648 Mar 199315 Mar 1994Thomson-CsfMethod for the directed modulation of the composition or doping of semiconductors, notably for the making of planar type monolithic electronic components, use of the method and corresponding products
US529845221 Feb 199229 Mar 1994International Business Machines CorporationMethod and apparatus for low temperature, low pressure chemical vapor deposition of epitaxial silicon layers
US530483415 Ene 199319 Abr 1994At&T Bell LaboratoriesSelective epitaxy of silicon in silicon dioxide apertures with suppression of unwanted formation of facets
US531045119 Ago 199310 May 1994International Business Machines CorporationMethod of forming an ultra-uniform silicon-on-insulator layer
US531695831 May 199031 May 1994International Business Machines CorporationMethod of dopant enhancement in an epitaxial silicon layer by using germanium
US533486119 May 19922 Ago 1994Motorola Inc.Semiconductor memory cell
US533690328 May 19939 Ago 1994North Carolina State University At RaleighSelective deposition of doped silicon-germanium alloy on semiconductor substrate, and resulting structures
US53468407 Dic 199213 Sep 1994Fujitsu LimitedMethod of producing heterojunction bipolar transistor having narrow band gap base type
US53468481 Jun 199313 Sep 1994Motorola, Inc.Method of bonding silicon and III-V semiconductor materials
US537456415 Sep 199220 Dic 1994Commissariat A L'Energie AtomiqueProcess for the production of thin semiconductor material films
US539337522 Dic 199328 Feb 1995Cornell Research Foundation, Inc.Process for fabricating submicron single crystal electromechanical structures
US53995228 Sep 199321 Mar 1995Fujitsu LimitedMethod of growing compound semiconductor
US541367930 Jun 19939 May 1995The United States Of America As Represented By The Secretary Of The NavyMethod of producing a silicon membrane using a silicon alloy etch stop layer
US54242439 Sep 199413 Jun 1995Fujitsu LimitedMethod of making a compound semiconductor crystal-on-substrate structure
US54260699 Abr 199220 Jun 1995Dalsa Inc.Method for making silicon-germanium devices using germanium implantation
US54263168 Jun 199420 Jun 1995International Business Machines CorporationTriple heterojunction bipolar transistor
US54422059 Ago 199315 Ago 1995At&T Corp.Semiconductor heterostructure devices with strained semiconductor layers
US546124329 Oct 199324 Oct 1995International Business Machines CorporationSubstrate for tensilely strained semiconductor
US546125010 Ago 199224 Oct 1995International Business Machines CorporationSiGe thin film or SOI MOSFET and method for making the same
US546288311 Abr 199431 Oct 1995International Business Machines CorporationMethod of fabricating defect-free silicon on an insulating substrate
US547681314 Nov 199419 Dic 1995Kabushiki Kaisha ToshibaMethod of manufacturing a bonded semiconductor substrate and a dielectric isolated bipolar transistor
US547903327 May 199426 Dic 1995Sandia CorporationComplementary junction heterostructure field-effect transistor
US548466421 Ene 199416 Ene 1996Fujitsu LimitedHetero-epitaxially grown compound semiconductor substrate
US549675019 Sep 19945 Mar 1996Texas Instruments IncorporatedElevated source/drain junction metal oxide semiconductor field-effect transistor using blanket silicon deposition
US549677119 May 19945 Mar 1996International Business Machines CorporationMethod of making overpass mask/insulator for local interconnects
US551672123 Feb 199514 May 1996International Business Machines CorporationIsolation structure using liquid phase oxide deposition
US55232438 Jun 19944 Jun 1996International Business Machines CorporationMethod of fabricating a triple heterojunction bipolar transistor
US55235921 Feb 19944 Jun 1996Hitachi, Ltd.Semiconductor optical device, manufacturing method for the same, and opto-electronic integrated circuit using the same
US553471320 May 19949 Jul 1996International Business Machines CorporationComplementary metal-oxide semiconductor transistor logic using strained SI/SIGE heterostructure layers
US553636123 Ene 199516 Jul 1996Canon Kabushiki KaishaProcess for preparing semiconductor substrate by bonding to a metallic surface
US55407854 Abr 199430 Jul 1996International Business Machines CorporationFabrication of defect free silicon on an insulating substrate
US557137318 May 19945 Nov 1996Memc Electronic Materials, Inc.Method of rough polishing semiconductor wafers to reduce surface roughness
US557204315 May 19955 Nov 1996The Furukawa Electric Co., Ltd.Schottky junction device having a Schottky junction of a semiconductor and a metal
US559652713 Feb 199521 Ene 1997Nippon Steel CorporationElectrically alterable n-bit per cell non-volatile memory with reference cells
US56173515 Jun 19951 Abr 1997International Business Machines CorporationThree-dimensional direct-write EEPROM arrays and fabrication methods
US562452910 May 199529 Abr 1997Sandia CorporationDry etching method for compound semiconductors
US56309055 Jun 199520 May 1997The Regents Of The University Of CaliforniaMethod of fabricating quantum bridges by selective etching of superlattice structures
US56332026 Jun 199627 May 1997Intel CorporationHigh tensile nitride layer
US56591877 Jun 199519 Ago 1997International Business Machines CorporationLow defect density/arbitrary lattice constant heteroepitaxial layers
US565919412 Mar 199619 Ago 1997Mitsubishi Denki Kabushiki KaishaSemiconductor device having metal silicide film
US56839343 May 19964 Nov 1997Motorola, Inc.Enhanced mobility MOSFET device and method
US569886913 Sep 199516 Dic 1997Kabushiki Kaisha ToshibaInsulated-gate transistor having narrow-bandgap-source
US571045023 Dic 199420 Ene 1998Intel CorporationTransistor with ultra shallow tip and method of fabrication
US571441311 Dic 19953 Feb 1998Intel CorporationMethod of making a transistor having a deposited dual-layer spacer structure
US571477719 Feb 19973 Feb 1998International Business Machines CorporationSi/SiGe vertical junction field effect transistor
US572862316 Mar 199517 Mar 1998Nec CorporationMethod of bonding a III-V group compound semiconductor layer on a silicon substrate
US57395678 Nov 199414 Abr 1998Wong; Chun Chiu D.Highly compact memory device with nonvolatile vertical transistor memory cell
US575989819 Dic 19962 Jun 1998International Business Machines CorporationProduction of substrate for tensilely strained semiconductor
US577734718 Jul 19977 Jul 1998Hewlett-Packard CompanyVertical CMOS digital multi-valued restoring logic device
US578661216 Abr 199628 Jul 1998Mitsubishi Denki Kabushiki KaishaSemiconductor device comprising trench EEPROM
US57866148 Abr 199728 Jul 1998Taiwan Semiconductor Manufacturing Co., Ltd.Separated floating gate for EEPROM application
US579267930 Ago 199311 Ago 1998Sharp Kabushiki KaishaMethod for forming silicon-germanium/Si/silicon dioxide heterostructure using germanium implant
US58083444 Feb 199715 Sep 1998International Business Machines CorporationSingle-transistor logic and CMOS inverters
US582157730 Nov 199213 Oct 1998International Business Machines CorporationGraded channel field effect transistor
US64922167 Feb 200210 Dic 2002Taiwan Semiconductor Manufacturing CompanyMethod of forming a transistor with a strained channel
US66211311 Nov 200116 Sep 2003Intel CorporationSemiconductor transistor having a stressed channel
US66572766 Jun 20022 Dic 2003Advanced Micro Devices, Inc.Shallow trench isolation (STI) region with high-K liner and method of formation
US668296526 Mar 199827 Ene 2004Sony CorporationMethod of forming n-and p- channel field effect transistors on the same silicon layer having a strain effect
US676490819 Jun 200220 Jul 2004Advanced Micro Devices, Inc.Narrow width CMOS devices fabricated on strained lattice semiconductor substrates with maximized NMOS and PMOS drive currents
US687605313 Ago 19995 Abr 2005Intel CorporationIsolation structure configurations for modifying stresses in semiconductor devices
US688508423 Jul 200326 Abr 2005Intel CorporationSemiconductor transistor having a stressed channel
US692999217 Dic 200316 Ago 2005Advanced Micro Devices, Inc.Strained silicon MOSFETs having NMOS gates with work functions for compensating NMOS threshold voltage shift
US200201350418 Abr 200226 Sep 2002Mitsubishi Denki Kabushiki KaishaSemiconductor integrated circuit and semiconductor device
US200300803611 Nov 20011 May 2003Chau Robert S.Semiconductor transistor having a stressed channel
US2004002932329 Jun 200112 Feb 2004Shimizu AkihiroSemiconductor device and method for fabricating the same
US2004014253717 Ene 200322 Jul 2004Sharp Laboratories Of America, Inc.Strained-silicon channel CMOS with sacrificial shallow trench isolation oxide liner
US200601518329 Sep 200513 Jul 2006Chau Robert SSemiconductor transistor having a stressed channel
Otras citas
Referencia
1Aldrich et al., "Stability of C54 Titanium Germanosilicide on a Silicon-Germanium Alloy Substrate," Journal of Applied Physics, vol. 77, No. 10 (1995) 5107-5114.
2Antoniadis et al., "SOI Devices and Technology," SOI devices and technology, Neuilly sur Seine, France, (1999), pp. 81-87.
3Aoyama et al., "Facet formation mechanism of silicon selective epitaxial layer by Si ultrahigh vacuum chemical vapor deposition," Journal of Crystal Growth, 136 (1994), pp. 349-354.
4Armstrong et al., "Design of Si/SiGe Heterojunction Complementary Metal-Oxide-Semiconductor Transistors," IEDM Technical Digest (1995 International Electron Devices Meeting), pp. 761-764.
5Armstrong, "Technology for SiGe Heterostructure-Based CMOS Devices," Ph.D. Thesis, Massachusetts Institute of Technology, Department of Electrical Engineering and Computer Science (Jun. 30, 1999).
6Arst et al., "Surface planarity and microstructure of low temperature silicon SEG and ELO," Journal of Materials Research, vol. 6, No. 4 (Apr. 1991), pp. 784-791.
7Aubry-Fortuna et al., "Phase Formation and Strain Relaxation During Thermal Reaction of Zr and Ti with Strained Si1-x GexCy Epilayers," Journal of Applied Physics, vol. 88, Iss. 3 (2000), 1481-1423.
8Augendre, "Elevated Source/Drain by Sacrificial Selective Epitaxy fo rHigh Performance Deep Submicron CMOS: Process Window versus Complexity," IEEE Transactins on Electron Devices, vol. 47, No. 7 (Jul. 2000), pp. 1484-1491.
9Augusto et al., "Proposal for a New Process Flow for the Fabrication of Silicon-based Complementary MOD-MOSFETs without ion Implantation," Thin Solid Films, vol. 294, No. 1-2, pp. 254-257 (Feb. 15, 1997).
10Barradas et al., "RBS analysis of MBE-grown SiGe/(001) Si heterostructures with thin, high Ge content SiGe channels for HMOS transistors," Modern Physics Letters B, 2001 (abstract).
11Borenstein et al., "A New Ultra-Hard Etch-Stop Layer for High Precision Micromachining," Proceedings of the 1999 12th IEEE International Conference on Micro Electro Mechanical Systems (MEMs) (Jan. 17-21, 1999), pp. 205-210.
12Bouillon et al., "Search for the optimal channel architecture for 0.18/0.12 mum bulk CMOS experimental study," IEEE, (1996), pp. 21.2.1-21.2.4.
13Bruel et al., "(R)SMART CUT: A Promising New SOI Material Technology," Proceedings of the 1995 IEEE International SOI Conference (Oct. 1995), pp. 178-179.
14Bruel, "Silicon on Insulator Material Technology," Electronic Letters, vol. 31, No. 14 (Jul. 6, 1995), pp. 1201-1202.
15Bufler et al., "Hole transport in strained Si1-xGex alloys on Si1-yGey substrates," Journal of Applied Physics, vol. 84, No. 10 (Nov. 15, 1998), pp. 5597-5602.
16Burghartz et al., "Microwave Inductors and Capacitors in Standard Multilevel Interconnect Silicon Technology," IEEE Transactions on Microwave Theory and Techniques, vol. 44, No. 1 (Jan. 1996), pp. 100-104.
17Canaperi et al., "Preparation of a relaxed Si-Ge layer on an insulator in fabrication high-speed semiconductor devices with strained epitaxial films," Intern. Business Machines Corporation, USA, 2002 (abstract).
18Cao et al., "0.18-mm Fully-Depleted Silicon-on-Insulator MOSFET's," IEEE Electron Device Letters, vol. 18, No. 6 (Jun. 1997), pp. 251-253.
19Carlin et al., "High Efficiency GaAs-on-Si Solar Cells with High Voc Using Graded GeSi Buffers," IEEE (2000), pp. 1006-1011.
20Chang et al., "Selective Etching of SiGe/Si Heterostructures," Journal of the Electrochemical Society, No. 1 (Jan. 1991), pp. 202-204.
21Cheng et al., "Electron Mobility Enhancement in Strained-Si n-MOSFETs Fabricated on SiGe-on-Insulator (SGOI) Substrates," IEEE Electrron Device Letters, vol. 22, No. 7 (Jul. 2001), pp. 321-323.
22Cheng et al., "Relaxed Silicon-Germanium on Insulator Substrate by Layer Transfer," Journal of Electronic Materials, vol. 30, No. 12 (2001), pp. L37-L39.
23Chieh et al., "Low-Resistance Bandgap-Engineered W/Si1-xGex/Si Contacts," IEEE Electron Device Letters, vol. 17, No. 7 (Jul. 1996) pp. 360-362.
24Choi et al., "30nm ultra-thin body SOI MOSFET with selectively deposited Ge raised S/D," 58th Device Research Conference (2000) pp. 23-24.
25Choi et al., "Nanoscale Ultrathin Body PMOSFETs With Raised Selective Germanium Source/Drain," IEEE Electron Device Letters, vol. 22, No. 9 (Sep. 2001), pp. 447-448.
26Cullis et al., "Growth ripples upon strained SiGe epitaxial layers on Si and misfit dislocation interactions," Journal of Vacuum Science and Technology A, vol. 12, No. 4 (Jul./Aug. 1994), pp. 1924-1931.
27Currie et al., "Carrier mobilities and process stability of strained Si n- and p-MOSFETs on SiGe virtual substrates," Journal of Vacuum Science and Technology B, vol. 19, No. 6 (Nov./Dec. 2001), pp. 2268-2279.
28Detavernier et al., "CoSi2 Nucleation in the Presence of Ge," Thin Solid Films, vol. 384, No. 2 (2001), pp. 243-250.
29Drowley et al., "Model for facet and sidewall defect formation during selective epitaxial growth of (001) silicon," Applied Physics Letters, 52 (7) (Feb. 15, 1988), pp. 546-548.
30Eaglesham et al., "Dislocation-Free Stranski-Krastanow Growth of Ge on Si(100)," Physical Review Letters, vol. 64, No. 16, (Apr. 16, 1990), pp. 1943-1946.
31Eaglesham et al., "Growth Morphology and the Equilibrium Shape: The Role of"Surfactants" in the Ge/Si Island Formation," Physical Review Letters, vol. 70, No. 7 (Feb. 15, 1993), pp. 966-969.
32Eberhart et al., "Ni/Ag Metallization for SiGe HBTs using a Ni Silicide Contact," Semiconductor Science and Technology vol. 16, No. 9, (2001) pp. L47-L49.
33Feijoo et al., "Epitaxial Si-Ge Etch Stop Layers with Ethylene Diamine Pyrocatechol for Bonded and Etchback Silicon-on-Insulator," Journal of Electronic Materials, vol. 23, No. 6 (Jun. 1994), pp. 493-496.
34Fischetti et al., "Band structure, deformation potentials, and carrier mobility in strained Si, Ge, and SiGe alloys," Journal of Applied Physics, vol. 80, No. 4 (Aug. 15, 1996), pp. 2234-2252.
35Fischetti, "Long-range Coulomb interactions i small Si devices. Part II. Effective electronmobility in thin-oxide structures," Journal of Applied Physics, vol. 89, No. 2 (Jan. 15, 2001), pp. 1232-1250
36Fitzgerald et al., "Dislocation dynamics in relaxed graded composition semiconductors," Materials Science and Engineering, B67 (1999), pp. 53-61.
37Fitzgerald et al., "Relaxed GexSi1-x structures for III-V integration with Si and high mobility two-dimensional electron gases in Si," Journal of Vacuum Science and Technology, (Jul./Aug. 1992), pp. 1807-1819.
38Fitzgerald et al., "Totally Relaxed GexSi1-x Layers with Low Threading Dislocation Densities Grown on Si Substrates," Applied Physics Letters, vol. 59, No. 7 (Aug. 12, 1991), pp. 811-813.
39Freiman et al., "Kinetics of Processes in the Ti-Si1-x Gex Systems," Applied Physics Letters vol. 69, No. 25 (1996) pp. 3821-3823.
40Freiman et al., "Titanium Metallization of Si/Ge Alloys and Superlattices," Thin Solid Films vol. 294, No. 1-2 (1997) pp. 217-219.
41Gallas et al., "Influence of doping on facet formation at the SiO2/Si interface," Surface Science, 440 (1999), pp. 41-48.
42Garone et al., "Silicon vapor phase epitaxial growth catalysis by the presence of germane," Applied Physics Letters, vol. 56, No. 13 (Mar. 26, 1990), pp. 1275-1277.
43Glück et al., "CoSi2 and TiSi2 for Si/SiGe heterodevices," Thin Solid Films, vol. 270 (1995) pp. 549-554.
44Godbey et al., (1990) "Fabrication of Bond and Etch-Back Silicon Insulator Using a Strained SI0.7GE0.3 Layer as an Etch Stop," Journal of the Electrical Society, vol. 137, No. 10 (Oct. 1990) pp. 3219-3223.
45Goulding, "The selective epitaxial growth of silicon," Materials Science and Engineering, B17 (1993), pp. 47-67.
46Gray et al., "Analysis and Design of Analog Integrated Circuits," John Wiley & Sons, 1984, pp. 605-632.
47Greve et al., "Growth Rate of Doped and Undoped Silicon by Ultra-High Vacuum Chemical Vapor Deposition," Journal of the Electrochemical Society, vol. 138, No. 6 (Jun. 1991), pp. 1744-1748.
48Grillot et al., "Acceptor diffusion and segregation in (AIxGa1-x)0.5In0.5P heterostructures," Journal of Applied Physics, vol. 91, No. 8 (2002), pp. 4891-4899.
49Grützmacher et al., "Ge segregation in SiGe/Si heterostructures and its dependence on deposition technique and growth atmosphere," Applied Physics Letters, vol. 63, No. 18 (Nov. 1, 1993), pp. 2531-2533.
50Hackbarth et al, "Alternatives to Thick MBE-Grown Relaxed SiGe Buffers," Thin Solid Films, vol. 369, pp. 148-151 (2000).
51Hackbarth et al., "Strain relieved SiGe buffers for Si-based heterostructure field-effect transistors," Journal of Crystal Growth, vol. 201/202 (1999), pp. 734-738.
52Halsall et al., "Electron diffraction and Raman studies of the effect of substrate misorientation on ordering in the AlGaInP system," Journal of Applied Physics, vol. 85, No. 1 (1999), pp. 199-202.
53Herzog et al., "SiGe-based FETs: Buffer Issues and Device Results," Thin Solid Films, vol. 380, No. 1-2, pp. 36-41 Dec. 12, 2000.
54Höck et al., "Carrier mobilities in modulation doped Si1-xGex heterostructures with respect to FET applications," Thin Solid Films, vol. 336 (1998), pp. 141-144.
55Höck et al., "High hole mobility in Si0.17 Ge0.83 channel metal-oxide-semiconductor field-effect transistors grown by plasma-enhanced chemical vapor deposition," Applied Physics Letters, vol. 76, No. 26 (Jun. 26, 2000), pp. 3920-3922.
56Höck et al., "High performance 0.25 mum p-type Ge/SiGe MODFETs," Electronics Letters, vol. 34, No. 19 (Sep. 17, 1998), pp. 1888-1889.
57Hsiao et al., "Advanced Technologies for Optimized Sub-Quarter-Micrometer SOI CMOS Devices," IEEE Transactions on Electron Devices, vol. 45, No. 5 (1998) pp. 1092-1098.
58Hsu et al., "Surface morphology of related GexSi1-x films," Appl. Phys. Lett., vol. 61, No. 11 (1992), pp. 1293-1295.
59Huang et al., "Electrical and Compositional Properties of Co-Silicided Shallow P+-n Junction Using Si-Capped/Boron-Doped Si1-xGex Layer Deposited by UHVCME," Journal of the Electrochemical Society, vol. 148, No. 3 (2001) pp. G126-C131.
60Huang et al., "High-quality strain-relaxed SiGe alloy grown on implanted silicon-on-insulator substrate," Applied Physics Letters, vol. 76, No. 19 (May 8, 2000), pp. 2680-2682.
61Huang et al., "The Impact of Scaling Down to Deep Submicron on CMOS RF Circuits," IEEE Journal of Solid-State Circuits, vol. 33, No. 7 (Jul. 1998), pp. 1023-1036.
62Huang et al., (2001) "Carrier Mobility enhancement in strained Si-on-insulatoir fabricated by wafer bonding", 2001 Symposium on VLSI Technology, Digest of Technical Papers, pp. 57-58.
63Huang, et al., "Study on Ge/Si Ration Silidation, and Strain Relaxation of High Temperature Sputtered Co/Si1-x Gex Structures," Journal of Applied Physics, vol. 88, No. 4 (2000) pp. 1831-1837.
64IBM Technical Disclosure Bulletin, "2 Bit/Cell EEPROM Cell Using Band to Band Tunneling for Data Read-Out," vol. 35, No. 4B (Sep. 1992), pp. 136-140.
65IBM Technical Disclosure Bulletin, "Optimal Growth Technique and Structure for Strain Relaxation of Si-Ge Layers on Si Substrates," vol. 32, No. 8A (Jan. 1990), pp. 330-331.
66Ilderem et al., "Very low pressure chemical vapor deposition process for selective titanium silicide films," Appl. Phys. Lett., vol. 53, No. 8 (Aug. 22, 1988) pp. 687-689.
67Ishikawa et al., "Creation of Si-Ge-based SIMOX structures by low energy oxygen implantation," Proceedings of the 1997 IEEE International SOI Conference (Oct. 1997), pp. 16-17.
68Ishikawa et al., "SiGe-on-insulator substrate using SiGe alloy grown Si(001)," Applied Physics Letters, vol. 75, No. 7 (Aug. 16, 1999), pp. 983-985.
69Ishitani et al., "Facet Formation in Selective Silicon Epitaxial Growth," Japanese Journal of Applied Physics, vol. 24, No. 10 (Oct. 1985), pp. 1267-1269.
70Ismail et al., "Modulation-doped n-type Si/SiGe with Inverted Interface," Applied Physics Letters, 65 (10), pp. 1248-1250 Sep. 5, 1994.
71Ismail, "Si/SiGe High-Speed Field-Effect Transistors," International Electron Devices Meeting, Washington, D.C. (Dec. 10, 1995), pp. 20.1.1-20.1.4.
72Ito, Shinya, IEEE, Mechanical stress effect of etch-stop nitride and its impact on deep submicron transistor design, http://ieeexplore.ieee.org/iel5/7241/19535/00904303.pdf?tp=&isnumber=&arnumber=904303.
73Jang et al., "Phosphorus doping of epitaxial Si and Si1-xGex at very low pressure," Applied Physics Letters, 63 (12) (Sep. 20, 1993), pp. 1675-1677.
74Jastrzebski, "SOI by CVD: Epitaxial Lateral Overgrowth (ELO) Process-Review," Journal of Crystal Growth, 63 (1983), pp. 493-526.
75Jungemann et al., "Full-Band Monte Carlo Simulation of a 0.12 mum-Si-PMOSFET with and without a Strained SiGe-Channel", IEEE Electron Devices Meeting, 1998, pp. 897-900.
76Kamins et al., "Kinetics of selective epitaxial deposition of Si1-xGex," Applied Physics Letters, 61 (6) (Aug. 10, 1992), pp. 669-671.
77Kandel et al., "Surfactant Mediated Crystal Growth of Semiconductors," Physical Review Letters, vol. 75, No. 14 (Oct. 2, 1995), pp. 2742-2745.
78Kearney et al., "The effect of alloy scattering on the mobility of holes in a Si1-xGex quantum well," Semiconductor Science and Technology, vol. 13 (1998), pp. 174-180.
79Kim et al., "A Fully Integrated 1.9-GHz CMOS Low-Noise Amplifier," IEEE Microwave and Guided Wave Letters, vol. 8, No. 8 (Aug. 1998), pp. 293-295.
80King et al., "A Polycrystalline Si1-xGex-Gate CMOS Technology", IEEE, vol. No. 1990, pp. 253-256.
81King, "Silicon-Germanium: from Microelectronics to Micromechanics," Presentation to the Thin Film Users Group Meeting, AVS Northern California Chapter, Apr. 17, 2002.
82Kitajima et al., "Lattice Defect in Selective Epitaxial Silicon and Laterally Overgrown Regions on SiO2," Journal of Crystal Growth, 98 (1989), pp. 264-276.
83Koester et al., "Extremely High Transconductance Ge/Si0.4Ge0.6 p-MODFET's Grown by UHV-CVD," IEEE Electron Device Letters, vol. 21, No. 3 (Mar. 2000), pp. 110-112.
84Konig et al., "Design Rules for N-Type SiGe Hetero FETs," Solid State Electronics, vol. 41, No. 10, pp. 1541-1547 Oct. 1, 1997.
85König et al., "p-Type Ge-Channel MODFET's with High Transconductance Grown on Si Substrates," IEEE Electron Device Letters, vol. 14, No. 4 (Apr. 1993), pp. 205-207.
86König et al., "SiGe HBTs and HFETs," Solid-State Electronics, vol. 38, No. 9 (1995), pp. 1595-1602.
87Ku et al., "High Performance PMOSFETS With Ni(Si1-x Gex )/Poly-Si0.8Ge0.2 Gate," IEEE- 2000 Symposium on BLSI Technology Digest of Technical Papers, pp. 114-115 (2000).
88Kurosawa et al., "A New Bird's Beak Free Field Isolation Technology for VLSI Devices," IEDM Technical Digest, Washington, D.C., Dec. 7-9, 1981, pp. 384-387.
89Kuznetsov et al., "Technology for high-performance n-channel SiGe modulation-doped field-effect transistors," J. Vac. Sci. Technol., B 13(6), pp. 2892-2896 (Nov./Dec. 1995).
90Lai, J.B. et al., "Effects of Composition on the Formation Temperatures and Electrical Resistivities of C54 Titanium Germanosilicide in Ti- Si1-x Gex Systems," Journal of Applied Physics, vol. 86, No. 3 (1999) pp. 1340-1345.
91Langdo et al., (2002) "Preparation of Novel SiGe-free Strained Si on Insulator Substrates" IEEE International SOI Conference, pp. 211-212 (XP002263057).
92Langdo, "Selective SiGe Nanostructures," Ph.D. Thesis, Massachusetts Institute of Technology, 2001.
93Larson, "Integrated Circuit Technology Options for RFIC's-Present Status and Future Directions," IEEE Journal of Solid-State Circuits, vol. 33, No. 3 (Mar. 1998), pp. 387-399.
94Lee et al., "CMOS RF Integrated Circuits at 5 GHz and Beyond," Proceedings of the IEEE, vol. 88, No. 10 (Oct. 2000), pp. 1560-1571.
95Lee et al., "Strained Ge channel p-type metal-oxide-semiconductor field-effect transistors grown on Si1-xGex/Si virtual substrates," Applied Physics Letters, vol. 79, No. 20 (Nov. 12, 2001), pp. 3344-3346.
96Lee et al., "Strained Ge channel p-type MOSFETs fabricated on Si1-xGex/Si virtual substrates," Material Research Society Symposium Proceedings, vol. 686 (2002), pp. A1.9.1-A1.9.5.
97Leitz et al., "Channel Engineering of SiGe-Based Heterostructures for High Mobility MOSFETs," Material Research Society Symposium Proceedings, vol. 686 (2002), pp. A3.10.1-A3.10.6.
98Leitz et al., "Dislocation glide and blocking kinetics in compositionally graded SiGe/Si," Journal of Applied Physics, vol. 90, No. 6 (Sep. 15, 2001), pp. 2730-2736.
99Leitz et al., "Hole mobility enhancements in strained Si/Si1-yGeyp-type metal-oxide-semiconductor field-effect transistors grown on relaxed Si1-xGex (x<y) virtual substrates," Applied Physics Letters, vol. 79, No. 25 (Dec. 17, 2001), pp. 4246-4248.
100Li et al., "Design of high speed Si/SiGe heterojunction complementary metal-oxide-semiconductor field effect transistors with reduced short-channel effects," Vacuum Science and Technology A, vol. 20, No. 3 (May/Jun. 2002), pp. 1030-1033.
101Mizuno, Tomohisa, IEEE, Novel SOI p-Channel MOSFETs With Higher Strain in Si Channel Using Double SiGe Heterostructures, Jan. 2002, http://ieeexplore.ieee.org/iel5/16/21019/00974741.pdf.
102Ota, K, IEEE, Novel Locally Strained Channel Technique for High Performance 55nm CMOS, http://ieeexplore.ieee.org/iel5/8330/25999/01175771.pdf?tp=&isnumber=&arnumber=1175771.
103Scott, Gregory, IEEE, NMOS Drive Current Reduction Caused by Transistor Layout and Trench Isolation Induced Stress, http://ieeexplore.ieee.org/iel5/6669/17838/00824277.pdf?tp=&arnumber=824277&isnumber=17838.
104Sleight, Jeffrey, IEEE, Stress Induced Defects and Transistor Leakage for Shallow Trench Isolated SOI, May 1999, http://ieeexplore.ieee.org/iel4/55/16464/00761029.pdf?tp=&isnumber=&arnumber=761029.
105Steegan, An, IEEE, Silicide Induced Pattern Density and Orientation Dependent Transconductance in MOS Transistors, http://ieeexplore.ieee.org/iel5/6669/17838/00824201.pdf?tp=&arnumber=824201&isnumber=17838.
106Wolf and Tauber, Silicon Processing for the VLSI Era: vol. 1-Process Technology, 2nd Edition, 2000, p. 203, Table 6-3.
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